张亦良, 刘金艳, 徐学东. 不锈钢X射线应力测量[J]. 北京工业大学学报, 2010, 36(9): 1165-1173.
    引用本文: 张亦良, 刘金艳, 徐学东. 不锈钢X射线应力测量[J]. 北京工业大学学报, 2010, 36(9): 1165-1173.
    ZHANG Yi-liang, LIU Jin-yan, XU Xue-dong. X-ray Stress Measurement of Stainless Steel[J]. Journal of Beijing University of Technology, 2010, 36(9): 1165-1173.
    Citation: ZHANG Yi-liang, LIU Jin-yan, XU Xue-dong. X-ray Stress Measurement of Stainless Steel[J]. Journal of Beijing University of Technology, 2010, 36(9): 1165-1173.

    不锈钢X射线应力测量

    X-ray Stress Measurement of Stainless Steel

    • 摘要: 分析了2类不锈钢X射线的衍射特性.为判断奥氏体不锈钢扫描过程中出现的2个衍射峰能否作为应力测试的基础,在改建的残余应力测量平台上,应用自编的测量控制软件,基于衍射全过程的实时监测与处理功能,采用等强梁标定方法,对奥氏体不锈钢0Cr18Ni9(原始材料)、1Cr18Ni9Ti (去应力退火)及马氏体不锈钢(A335P92)3种材料进行多次测定,逐级加载的同时,分别采用X射线系统及电测法进行检测,通过与理论值进行综合对比,得出不锈钢的衍射特性.结果表明:奥氏体与马氏体不锈钢反映了不同的衍射特性;虽然奥氏体不锈钢(220)晶面127°的Kα衍射峰非常明显,且半高宽与抛物线2种定峰方法的精确度较高,但准确度差,由此峰计算出的应力与材料真实应力无关;而(311)晶面149°的Kβ衍射峰虽然峰背比低、误差偏大,但经过应力常数修正后可作为应力测定依据;马氏体不锈钢表现出与α-Fe相近的衍射特性,其标定的应力常数与常规α-Fe的应力常数相差7.8%.

       

      Abstract: The diffraction properties of two types stainless stain were discussed.To clarify whether the two diffraction peaks during the process of 2θ scanning of austenite stainless steel diffraction,can be the basis of the stress measurement,two different austenite stainless steels—0Cr18Ni9(raw material),1Cr18Ni9Ti(stress relief annealing) and martensitc stainless stain.(A335P92) were measured for many times in this paper.They were demarcated by equal intensity girder method and detected by X-ray system and electromotive method respectively when gradually loaded by using a modified residual stress detecting equipment,self-edit measuring software and based on the monitoring and disposingl function in spots during diffracting process.Then the X-ray diffraction characteristics were obtained by comparing with theoretical values.The results show that austenite and martensitic stainless steel reflect the different characteristics of the diffraction.Although at 127°,corresponding to crystal face(220),Kα diffraction peak of austenite stainless steel is strikingly marked,and two peak locations—the half-width and parabola are accurate,the precision is poor and the stress calculated from this peak does not represent the actual stress according to this peak.However,although Kβ diffraction peak at 149°,corresponding to crystal face(311),in spite of the lower peak-back ratio,149° Kβ can be the basis to calculate stress after the stress constant was modified.Martensitic stainless steel shows the diffraction properties which are close to that of α-Fe,and the difference between the stress constant acquired by martensitic stainless steel calibration and that of conventional α-Fe is 7.8%.

       

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